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CHEM01200604005 A. K. Pathak - Homi Bhabha National Institute

CHEM01200604005 A. K. Pathak - Homi Bhabha National Institute

CHEM01200604005 A. K. Pathak - Homi Bhabha National Institute

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The structures of the hydrated cluster, CO • 3 ⎯.nH 2 O (n=1-8) are calculated at<br />

B3LYP/6-311++G(d,p) level of theory and discussed in Chapter 2. Similarly various<br />

possible initial structures of CO •− 3 .nH 2 O (n=1-8) clusters are considered for global<br />

geometry optimization and a number of minimum energy structures (conformers) are<br />

obtained. Fully optimized global minimum energy structure of each size of hydrated<br />

cluster, CO •− 3 .nH 2 O (n=1-8) at B3LYP/6-311++G(d,p) level is displayed in Fig. 5.2.<br />

These structures of the hydrated cluster, CO • 3 ⎯.nH 2 O are very close to that discussed in<br />

Chapter 2.<br />

It is observed that CO • 3 ⎯.nH 2 O clusters are stabilized by double hydrogen bonding<br />

(DHB), single hydrogen bonding (SHB) as well as inter water hydrogen bonding (WHB).<br />

In each case, the distance between the C and O atoms of carbonate moiety (CO • 3 ⎯) is ~<br />

1.3 Å. The calculated distance between O (of CO • 3 ⎯) and H-bonded H atoms is 1.8-2.2 Å<br />

(SHB and DHB bond) and the distance between O and H atoms in inter water network is<br />

1.9-2.1 Å (WHB bond). It is worth to mention that the globally optimized structures for<br />

both the cases are very close to that of most stable structure as discussed in Chapter 2.<br />

5.3.2. UV-Vis Spectra<br />

Calculations are performed to find out a few low lying excited states for all the<br />

solvated clusters as well as for the isolated dimer radical anion (Cl •− 2 ) at both CIS and<br />

TDDFT level of theory to observe the shift in optical absorption wavelength (l) of the<br />

dimer radical anion (Cl •− 2 ) with addition of solvent water molecules. The absorption<br />

maxima (λ max ) for isolated dimer radical anion (Cl •− 2 ) is found to be at 437 nm at CIS/6-<br />

89

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